The full-wedge rotation of \(\mathbf {Q}\)  is defined as [1]}
\({\left\lbrace \begin{array}{ll}\Delta \Gamma /2=\cos (\Omega \tau )\\\Xi =|\sin (\Omega \tau )| \\\phi _{d}=\left[H(\tau -T/2)-1/2\right]\Delta \phi _d,\end{array}\right.}\) 
